c which is only exceeded by cuprates.
This has raised question about whether these systems are
conventional superconductors.
Important parameters for fullerides are the effective Coulomb
repulsion U between two electrons on the same molecule, the
one-electron band width W of the partly occupied t1u
band, the maximum phonon frequency wph, the
Jahn-Teller energy EJT and the exchange integral K.
Typical estimates of these parameters are
U | 1.0-1.5 eV |
W | 0.6 eV |
wph | 0.2 eV |
EJT | 0.1 eV |
K | 0.1 eV |
This leads to interesting questions:
1. Since U>W, one might have expected all
AnC60
compounds to be insulators, while experimentally
A3C60
are metals and
A4C60
are insulators.
2. Migdal's theorem plays an important role in the theory of conventional
superconductors. Since, however, wph is similar
to W, it is questionable if this theorem is valid for the fullerides.
3. The superconductivity is driven by the electron-phonon interaction,
which induces an attractive interaction of the order 0.1 eV. At the
same time there is a repulsive Coulomb repulsion U of the order
1 to 1.5 eV. In conventional superconductors this repulsion is believed
to be drastically reduced by retardation effects, due to the vastly
different energy scales of the electrons and phonons. Here
wph and W are comparable, which raises basic
questions about why superconductivity is at all possible.
4. For large temperatures the resistivity becomes very large and the
corresponding mean free path much shorter than the separation
between two molecules. This raises interesting questions
about the interpretation and whether such a result is even possible.
The unusual resistivity is related to the small band width.
5. There is an interesting competition between the Jahn-Teller effect,
the Hund's rule coupling, the kinetic and the Coulomb energies.
Since these issues emphasize the many-body nature of the
problem and since
AnC60
is very complicated, our work is mainly based on model calculations.
For this purpose we have constructed appropriate models and
determined the corresponding parameters from ab initio calculations
or experiments. The models are solved by using Quantum Monte-Carlo
(T=0 projection and finite T determinantal) methods,
dynamical mean-field theory or exact diagonalization
techniques.
Among the issues treated are:
Models and parameters
Superconductivity
Metal-insulator transition
Resistivity
Electron-phonon interaction
Coulomb pseudopotential
Jahn-Teller effect
Plasmons
Screening
Susceptibility
Photoemission
Orientational interaction
Electronic structure
Optical conductivity
Raman scattering
NMR
Electron density of states
Fullerene molecules
Properties of A3C60
have been discussed extensively in the book "Alkali-doped Fullerides.
Narrow-band solids with unusual properties"
(
World Scientific, Singapore, 2004. XVII, 282 p., hardcover. ISBN 981-238-667-X
). Also available at
Amazon.
Superconductivity properties have been reviewed in
"Superconductivity in Fullerides"
(
Rev. Mod. Phys. 69, 575 (1997)).
A list of some relevant
publications is given.
For further information contact Olle Gunnarsson (o.gunnarsson@fkf.mpg.de)
or Erik Koch (E.Koch@fz-juelich.de).
Last Update: October 2010
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